JP5703930B2 - OPTICAL SYSTEM, IMAGING DEVICE HAVING THE OPTICAL SYSTEM, AND OPTICAL SYSTEM MANUFACTURING METHOD - Google Patents

Description

  The present invention relates to an optical system, an imaging apparatus having the optical system, and a method for manufacturing the optical system.

  Conventionally, many so-called modified Gaussian lenses have been proposed (see, for example, Patent Document 1).

JP 2009-251398 A

  However, the conventional Gaussian lens has insufficient correction of coma, and it has been particularly difficult to improve sagittal coma.

  The present invention has been made in view of such a problem, and is an optical system that is small in size, has a small number of components, has high performance, has low coma aberration, particularly sagittal coma aberration, and spherical aberration, and an imaging apparatus having the optical system. And it aims at providing the manufacturing method of an optical system.

In order to solve the above-described problem, the optical system according to the present invention includes substantially two lens groups of a front group and a rear group having a positive refractive power in order from the object side along the optical axis. The front group includes, in order from the object side, a first lens component having a positive refractive power, a second lens component having a negative refractive power and a convex surface facing the object side, and a first lens component having a negative refractive power. It consists of a third lens component, the rear group includes, in order from the object side, is joined with a negative lens and a positive lens having a first lens component having a concave surface facing the object side, a positive refractive power, the image side a second lens component having a concave surface, and a third lens component having positive refractive power, and satisfies the following conditional expression.
0.000 <nRNP-nRNN <0.350
−2.00 <(rp2−rp1) / (rp2 + rp1) <− 0.00
However,
nRNP: Refractive index with respect to d-line of medium of positive lens in first lens component in rear group nRNN: Refractive index with respect to d-line of medium of negative lens in first lens component in rear group rp1: In rear group Radius of curvature of the surface closest to the object side of the second lens component rp2: radius of curvature of the surface closest to the image side of the second lens component in the rear group

Such an optical system preferably satisfies the following conditional expression.
0.00 <(− fFN1) / f0 <20.00
However,
fFN1: Focal length of the second lens component in the front group f0: Focal length of the entire system when focusing on infinity

Such an optical system preferably satisfies the following conditional expression.
0.20 <(-fFN2) / f0 <15.00
However,
fFN2: focal length of the third lens component in the front group f0: focal length of the entire system when focusing on infinity

In such an optical system, the second lens component in the rear group is preferably a cemented lens in which a positive lens and a negative lens are cemented, and preferably satisfies the following conditional expression.
0.000 <nRPP-nRPN <0.500
However,
nRPP: refractive index of the second lens component in the rear group with respect to the d-line of the medium of the positive lens nRPN: refractive index of the second lens component in the rear group with respect to the d-line of the medium of the negative lens

Such an optical system preferably satisfies the following conditional expression.
1.00 <fRP / f0 <12.00
However,
fRP: focal length of the second lens component in the rear group f0: focal length of the entire system when focusing on infinity

Such an optical system preferably satisfies the following conditional expression.
0.1 <fRP2 / f0 <3.0
However,
fRP2: focal length of the third lens component in the rear group f0: focal length of the entire system when focusing on infinity

  In such an optical system, the front group preferably has at least one aspheric surface.

  In such an optical system, the rear group preferably has at least one aspheric surface.

  In such an optical system, the third lens component in the rear group is preferably a positive lens having a convex surface facing the object side.

  Such an optical system preferably has an aperture stop between the front group and the rear group.

  In addition, an imaging apparatus according to the present invention includes any one of the above-described optical systems.

In addition, the method of manufacturing an optical system according to the present invention is an optical system including substantially two lens groups , a front group and a rear group having a positive refractive power, in order from the object side along the optical axis. In the manufacturing method, as a front group, in order from the object side, a first lens component having a positive refractive power, a second lens component having a negative refractive power and having a convex surface facing the object side, and a negative lens A third lens component having a refractive power, and as a rear group, a negative lens and a positive lens are joined in order from the object side, and a first lens component having a concave surface facing the object side, and a positive refractive power And a second lens component having a concave surface facing the image side and a third lens component having a positive refractive power are disposed, and the following conditional expression is satisfied.
0.000 <nRNP-nRNN <0.350
−2.00 <(rp2−rp1) / (rp2 + rp1) <− 0.00
However,
nRNP: Refractive index with respect to d-line of medium of positive lens in first lens component in rear group nRNN: Refractive index with respect to d-line of medium of negative lens in first lens component in rear group rp1: In rear group Radius of curvature of the surface closest to the object side of the second lens component rp2: radius of curvature of the surface closest to the image side of the second lens component in the rear group

  According to the present invention, there are provided an optical system that is small in size, has a small number of components, has high performance, and has low coma, particularly sagittal coma and spherical aberration, an imaging apparatus having the optical system, and a method for manufacturing the optical system. be able to.

It is sectional drawing which shows the lens structure in the infinite point focusing state of the optical system which concerns on 1st Example. FIG. 6 is a diagram illustrating various aberrations of the optical system according to Example 1 in an infinitely focused state. It is sectional drawing which shows the lens structure in the infinite point focusing state of the optical system which concerns on 2nd Example. FIG. 10 is a diagram illustrating various aberrations of the optical system according to Example 2 in a focused state at infinity. It is sectional drawing which shows the lens structure in the infinite point focusing state of the optical system which concerns on 3rd Example. FIG. 11 is a diagram illustrating various aberrations of the optical system according to Example 3 in an infinitely focused state. It is sectional drawing which shows the lens structure in the infinite point focusing state of the optical system which concerns on 4th Example. FIG. 11 is a diagram illustrating various aberrations of the optical system according to Example 4 in the infinitely focused state. It is sectional drawing which shows the lens structure in the infinite point focusing state of the optical system which concerns on 5th Example. FIG. 11 is a diagram illustrating various aberrations of the optical system according to Example 5 in a focused state at infinity. It is sectional drawing which shows the lens structure in the infinite point focusing state of the optical system which concerns on 6th Example. It is various aberrational figures in the infinite point focusing state of the optical system which concerns on 6th Example. It is sectional drawing which shows the lens structure in the infinite point focusing state of the optical system which concerns on 7th Example. FIG. 10 is a diagram illustrating various aberrations of the optical system according to Example 7 in a focused state at infinity. It is sectional drawing which shows the lens structure in the infinite point focusing state of the optical system which concerns on 8th Example. It is various aberrational figures in the infinite point focusing state of the optical system which concerns on 8th Example. A sectional view of a single-lens reflex camera with an optical system is shown. It is a flowchart for demonstrating the manufacturing method of an optical system.

  Hereinafter, preferred embodiments of the present invention will be described with reference to the drawings. As shown in FIG. 1, the optical system OS according to the present embodiment includes a front group GF and a rear group GR having a positive refractive power in order from the object side along the optical axis. . The front group GF includes, in order from the object side, a first lens component LFP having a positive refractive power, a second lens component LFN1 having a negative refractive power and having a convex surface facing the object side, and negative refraction. The rear lens group GR has a first lens component LRN in which a negative lens L21 and a positive lens L22 are cemented in order from the object side, and a concave surface is directed to the object side. The lens includes a second lens component LRP1 having a positive refractive power and a concave surface facing the image side, and a third lens component LRP2 having a positive refractive power. In the following description, “lens component” refers to a single lens (lens element) or a cemented lens in which two or more single lenses (lens elements) are cemented.

  The optical system OS according to the present embodiment has coma aberration, particularly sagittal coma aberration, which is a defect of so-called Gaussian type and xenota type optical systems, which are basically represented by positive, negative, positive, negative, chromatic aberration, curvature of field and non-existence. This is an improvement without deteriorating the point aberration. Hereinafter, conditions for configuring such an optical system OS will be described.

  The optical system OS according to the present embodiment desirably satisfies the following conditional expression (1).

0.000 <nRNP-nRNN <0.350 (1)
However,
nRNP: refractive index with respect to the d-line of the medium of the positive lens L22 in the first lens component LRN in the rear group GR nRNN: refractive index with respect to the d-line of the medium of the negative lens L21 in the first lens component LRN in the rear group GR

  Conditional expression (1) is a condition that regulates the difference in refractive index between the positive lens L22 and the negative lens L21 constituting the first lens component LRN in the rear group GR at the d-line (wavelength λ = 587.6 nm). If this condition is not met, the setting of the optimum value for the Petzval sum will be impaired, resulting in a worsening of field curvature.

  If the upper limit value of the conditional expression (1) is exceeded, it means that the refractive index difference is remarkably increased. Even in this case, the Petzval sum is deteriorated from the optimum value, and as a result, the correction of the field curvature is deteriorated. In addition, the ability to correct spherical aberration also decreases, which makes it impossible to select a glass material for optimal chromatic aberration. If the upper limit value of conditional expression (1) is set to 0.300, the above-described correction of various aberrations becomes more advantageous. If the upper limit value of conditional expression (1) is set to 0.200, the above-described correction of various aberrations becomes more advantageous. Further, by setting the upper limit value of conditional expression (1) to 0.130, the effect of the present application can be maximized.

  If the lower limit of conditional expression (1) is not reached, the difference in refractive index becomes remarkably small, and finally the refractive index of the negative lens L21 becomes larger than the refractive index of the positive lens L22. In this case, the positive and negative refractive indexes are reversed, and it is difficult to keep the Petzval sum small. Accordingly, the Petzval sum deviates greatly from the optimum value, and as a result, correction of curvature of field and correction of astigmatism are deteriorated, which is not preferable. If the lower limit value of conditional expression (1) is set to 0.020, it is advantageous for correction of various aberrations such as field curvature and astigmatism. Setting the lower limit of conditional expression (1) to 0.035 is advantageous for correcting various aberrations such as field curvature and astigmatism. Further, by setting the lower limit value of conditional expression (1) to 0.05, the effect of the present application can be maximized.

  Moreover, it is desirable that the optical system OS according to the present embodiment satisfies the following conditional expression (2).

−2.00 <(rp2-rp1) / (rp2 + rp1) <− 0.00 (2)
However,
rp1: radius of curvature of the most object side surface of the second lens component LRP1 in the rear group GR rp2: radius of curvature of the most image side surface of the second lens component LRP1 in the rear group GR

  Conditional expression (2) is a condition that defines the reciprocal of the form factor of the entire second lens component LRP1 having a positive refractive power with the concave surface facing the image side in the rear group GR. This condition is greatly related to correction of spherical aberration and sagittal coma. The fact that the value set in the conditional expression (2) is negative means that the entire shape of the second lens component LRP1 with the concave surface facing the image side in the rear group GR is a positive lens component. However, it shows a negative meniscus shape. Due to the presence of the air lens formed between this shape and the positive lens component (third lens component LRP2) located on the image side, it is possible to satisfactorily correct sagittal coma, meridional coma, and spherical aberration.

  When the upper limit value of conditional expression (2) is exceeded, the second lens component LRP1 changes its shape greatly from the negative meniscus shape and is a positive meniscus shape with a convex surface facing the object side, or a negative meniscus with a concave surface facing the object side Become a shape. Regardless of which shape is reached, the correction of sagittal coma and meridional coma is deteriorated, and correction of spherical aberration is also undesirably deteriorated when trying to correct it satisfactorily. If the upper limit value of conditional expression (2) is set to -0.01, the above-described correction of various aberrations becomes more advantageous. If the upper limit value of conditional expression (2) is set to -0.03, it becomes more advantageous to correct the above-mentioned various aberrations. In addition, the effect of the present application can be maximized by setting the upper limit value of conditional expression (2) to -0.05.

  When the lower limit value of conditional expression (2) is not reached, the second lens component LRP1 is greatly changed from a negative meniscus shape to a biconvex shape or a biconcave shape. For this reason, the air lens described above does not exist, and the characteristics from the negative meniscus shape are not maintained, so that sagittal coma aberration, meridional coma aberration correction, and spherical aberration correction are deteriorated, which is not preferable. If the lower limit value of conditional expression (2) is set to -1.00, it is advantageous for correcting the above-mentioned various aberrations. Setting the lower limit of conditional expression (2) to −0.60 is advantageous for correcting the above-mentioned various aberrations. Moreover, the effect of the present application can be maximized by setting the lower limit value of conditional expression (2) to −0.40.

  In addition, it is desirable that the optical system OS according to the present embodiment satisfies the following conditional expression (3).

0.00 <(− fFN1) / f0 <20.00 (3)
However,
fFN1: focal length of the second lens component LFN1 in the front group GF f0: focal length of the entire system when focusing on infinity

  Conditional expression (3) is a condition that defines the combined focal length of the negative lens component (second lens component LFN1) with the convex surface facing the object side of the front group GF. The front group GF of the optical system OS according to the present embodiment has a positive and negative configuration, and defines the optimum refractive power of the negative lens component (second lens component LFN1) at the intermediate portion.

  When the upper limit value of the conditional expression (3) is exceeded, it means that the negative refractive power of the negative lens component (second lens component LFN1) becomes weak. In this case, correction of field curvature and astigmatism deteriorates, which is not preferable. When the upper limit value of conditional expression (3) is set to 15.00, the above-described correction of various aberrations becomes more advantageous. If the upper limit value of conditional expression (3) is set to 12.00, the above-described correction of various aberrations becomes more advantageous. Further, by setting the upper limit value of conditional expression (3) to 10.00, the effects of the present application can be maximized.

  Further, when the lower limit value of conditional expression (3) is not reached, it means that the negative refractive power of the negative lens component (second lens component LFN1) becomes strong. In that case, correction of coma aberration, spherical aberration, and distortion is deteriorated as a result, which is not preferable. If the lower limit value of conditional expression (3) is set to 0.30, it is advantageous for correction of various aberrations such as spherical aberration. Setting the lower limit value of conditional expression (3) to 0.59 is advantageous for correcting various aberrations such as spherical aberration. In addition, by setting the lower limit value of conditional expression (3) to 1.00, the effects of the present application can be maximized.

  In addition, it is desirable that the optical system OS according to the present embodiment satisfies the following conditional expression (4).

0.20 <(− fFN2) / f0 <15.00 (4)
However,
fFN2: focal length of the third lens component LFN2 in the front group GF f0: focal length of the entire system when focusing on infinity

  Conditional expression (4) is a condition that defines the magnitude of the focal length of the negative lens component (third lens component LFN2) on the image side of the front group GF, in other words, the magnitude of the negative refractive power.

  When the upper limit value of the conditional expression (4) is exceeded, it means that the negative refractive power of the negative lens component (third lens component LFN2) on the image side of the front group GF is reduced. In this case, the balance of correction for spherical aberration and coma is lost, which is not preferable. When the upper limit value of conditional expression (4) is set to 10.00, the above-described correction of various aberrations is advantageous. If the upper limit value of conditional expression (4) is set to 8.00, the above-described correction of various aberrations is advantageous. Further, by setting the upper limit value of conditional expression (4) to 7.00, the effect of the present application can be maximized.

  Further, when the lower limit value of conditional expression (4) is not reached, it means that the negative refractive power of the negative lens component (third lens component LFN2) on the image side of the front group GF is increased. This is not preferable because sagittal coma and distortion are particularly deteriorated. If the lower limit value of conditional expression (4) is set to 0.30, the above-mentioned various aberrations can be corrected more favorably. If the lower limit value of conditional expression (4) is set to 0.50, the above-mentioned various aberrations can be corrected more favorably. If the lower limit value of conditional expression (4) is set to 0.80, the above-mentioned various aberrations can be corrected more favorably. Further, by setting the lower limit value of conditional expression (4) to 0.86, the effect of the present application can be maximized.

  In the optical system OS according to the present embodiment, the second lens component LRP1 of the rear group GR is a cemented lens in which the positive lens L23 and the negative lens L24 are cemented, and satisfies the following conditional expression (5): It is desirable to do.

0.000 <nRPP-nRPN <0.500 (5)
However,
nRPP: refractive index of the second lens component LRP1 in the rear group GR with respect to the d-line of the medium of the positive lens L23 nRPN: refractive index of the medium of the negative lens L24 of the second lens component LRP1 in the rear group GR with respect to the d-line

  Conditional expression (5) is a condition that defines the relationship between the refractive indexes of the positive lens L23 and the negative lens L24 in the positive lens component (second lens component LRP1) in the rear group GR. Basically, the positive lens L23 has a higher refractive index than the negative lens L24, and the Petzval sum is suppressed to a small value.

  If the upper limit value of the conditional expression (5) is exceeded, the difference in refractive index between the positive lens L23 and the negative lens L24 becomes remarkably large, so that a dispersion difference cannot be secured with the currently existing glass material, and the correction of chromatic aberration deteriorates. If the upper limit value of conditional expression (5) is set to 0.400, the above-described correction of various aberrations becomes more advantageous. If the upper limit value of conditional expression (5) is set to 0.300, the above-described correction of various aberrations becomes more advantageous. Further, by setting the upper limit value of conditional expression (2) to 0.250, the effect of the present application can be maximized.

  When the lower limit of conditional expression (5) is not reached, the difference in refractive index between the positive lens L23 and the negative lens L24 becomes smaller, and the height is finally reversed. Since the refractive index of the negative lens L24 is higher than that of the positive lens L23, it becomes difficult to set an optimal value for the Petzval sum, and as a result, field curvature and astigmatism are deteriorated. If the lower limit value of conditional expression (5) is set to 0.100, it is advantageous for correcting the above-mentioned various aberrations. Setting the lower limit of conditional expression (5) to 0.130 is advantageous for correcting the above-mentioned various aberrations. Further, by setting the lower limit value of conditional expression (5) to 0.145, the effect of the present application can be maximized.

  In addition, it is desirable that the optical system OS according to the present embodiment satisfies the following conditional expression (6).

1.00 <fRP / f0 <12.00 (6)
However,
fRP: focal length of the second lens component LRP1 in the rear group GR f0: focal length of the entire system when focusing on infinity

  Conditional expression (6) is a condition that defines the combined focal length of the positive lens component (second lens component LRP1) with the concave surface facing the image side in the rear group GR. In the optical system OS according to the present embodiment, the rear group GR has a negative positive or positive configuration, and a positive lens component (second lens) disposed at the intermediate portion and having a concave surface facing the image side. It defines the optimum refractive power of the component LRP1).

  When exceeding the upper limit value of the conditional expression (6), it means that the focal length of the positive lens component (second lens component LRP1) is remarkably increased and the positive refractive power is weakened. In this case, the correction of sagittal coma, meridional coma, field curvature, and astigmatism deteriorates, which is not preferable. When the upper limit value of conditional expression (6) is set to 10.00, the above-described correction of various aberrations becomes more advantageous. If the upper limit value of conditional expression (6) is set to 9.00, the above-described correction of various aberrations becomes more advantageous. Further, by setting the upper limit value of conditional expression (6) to 8.00, the effect of the present application can be maximized.

  On the other hand, if the lower limit value of conditional expression (6) is not reached, it means that the focal length of the positive lens component (second lens component LRP1) is remarkably shortened and the positive refractive power is remarkably increased. In this case, the correction of spherical aberration, sagittal coma aberration, and meridional coma aberration deteriorates as a result, which is not preferable. Also, the sensitivity to eccentricity increases, which is not preferable. If the lower limit value of conditional expression (6) is set to 1.50, it is advantageous for correction of various aberrations such as spherical aberration. Setting the lower limit of conditional expression (6) to 1.92 is advantageous for correcting various aberrations such as spherical aberration. Further, by setting the lower limit value of conditional expression (6) to 2.75, the effect of the present application can be maximized.

  Moreover, it is desirable that the optical system OS according to the present embodiment satisfies the following conditional expression (7).

0.1 <fRP2 / f0 <3.0 (7)
However,
fRP2: focal length of the third lens component LRP2 in the rear group GR f0: focal length of the entire system when focusing on infinity

  Conditional expression (7) is a condition that defines the focal length of the positive lens component (third lens component LRP2) located on the image side in the rear group GR. In the optical system OS according to the present embodiment, the rear group GR has a negative positive or positive configuration, and an optimum refractive power of the positive lens component (third lens component LRP2) disposed on the image side. It prescribes.

  When the upper limit value of the conditional expression (7) is exceeded, it means that the focal length of the positive lens component (third lens component LRP2) is remarkably increased and the positive refractive power is weakened. In this case, the correction capability of spherical aberration and coma aberration is lowered, which is not preferable. If the upper limit value of conditional expression (7) is set to 2.5, the above-described correction of various aberrations becomes more advantageous. If the upper limit value of conditional expression (7) is set to 2.0, the above-described correction of various aberrations becomes more advantageous. In addition, the effect of the present application can be maximized by setting the upper limit value of conditional expression (7) to 1.5.

  If the lower limit value of conditional expression (7) is not reached, it means that the focal length of the positive lens component (third lens component LRP2) is remarkably shortened and the positive refractive power is remarkably increased. In this case, the correction of spherical aberration, sagittal coma aberration, and meridional coma aberration deteriorates as a result, which is not preferable. Also, the sensitivity to eccentricity increases, which is not preferable. If the lower limit value of conditional expression (7) is set to 0.2, it is advantageous for correction of various aberrations such as spherical aberration. Setting the lower limit of conditional expression (7) to 0.4 is advantageous for correcting various aberrations such as spherical aberration. Further, by setting the lower limit value of conditional expression (2) to 0.6, the effect of the present application can be maximized.

  The front group GF preferably has at least one aspheric surface, which is advantageous for correcting spherical aberration and coma corresponding to a large aperture. In addition, it is desirable that the rear group GR described above also has at least one aspheric surface. Similarly, the rear group GR is advantageous for correcting spherical aberration and coma corresponding to a large aperture. It should be noted that having one aspherical surface before and after the aperture stop S is effective in correcting aberrations caused by a large aperture such as spherical aberration, sagittal coma and meridional coma.

  The positive lens component (third lens component LRP2) disposed on the image side in the rear group GR is preferably a positive lens having a convex surface directed toward the object side. Combined with the positive lens component (second lens component LRP1) with the concave surface facing the image side in the rear group GR just before, a convex air lens can be made, which is advantageous for correcting spherical aberration and sagittal coma aberration. .

  In addition, an aperture stop S between the front group GF and the rear group GR is preferable for correcting lateral chromatic aberration and distortion.

  In the optical system OS according to the present embodiment, the first to third lens components LFP, LFN1, and LFN2 constituting the front group GF and the third lens component LRP2 constituting the rear group GR are shown in FIG. Although it is composed of a single lens, it may be composed of a cemented lens in which two or more single lenses are cemented.

  FIG. 17 is a schematic cross-sectional view of a single-lens reflex camera 1 (hereinafter simply referred to as a camera) as an imaging apparatus including the optical system OS described above. In this camera 1, light from an object (subject) (not shown) is collected by the taking lens 2 (optical system OS) and focused on the focusing screen 4 via the quick return mirror-3. The light imaged on the focusing screen 4 is reflected a plurality of times in the pentaprism 5 and guided to the eyepiece lens 6. Thus, the photographer can observe the object (subject) image as an erect image through the eyepiece 6.

  When the release button (not shown) is pressed by the photographer, the quick return mirror 3 is retracted out of the optical path, and the light of the object (subject) (not shown) condensed by the taking lens 2 is captured by the image sensor 7. A subject image is formed on the top. Thereby, the light from the object (subject) is captured by the image sensor 7 and recorded as an object (subject) image in a memory (not shown). In this way, the photographer can shoot an object (subject) with the camera 1. In addition, the camera 1 shown in FIG. 17 may hold | maintain the photographic lens 2 so that attachment or detachment is possible, and may be integrally molded with the photographic lens 2. Further, the camera 1 may be a so-called single-lens reflex camera, or a compact camera without a quick return mirror or a mirrorless single-lens reflex camera.

  Here, by mounting the above-described optical system OS as the photographing lens 2 on the camera 1, a large-aperture lens with less spherical aberration, sagittal coma flare, field curvature, and coma is realized by its characteristic lens configuration. doing. As a result, the camera 1 can realize an image pickup apparatus that has a large aperture and is capable of wide-angle shooting with less spherical aberration, sagittal coma aberration, field curvature, and meridional coma aberration.

  In addition, the contents described below can be employed as appropriate within a range that does not impair the optical performance.

  In the present embodiment, the optical system OS having the two-group configuration is shown, but the above-described configuration conditions and the like can be applied to other group configurations such as the third group, the fourth group, and the like. Further, a configuration in which a lens or a lens group is added closest to the object side, a configuration in which a lens or a lens group is added closest to the image side, or a configuration in which a lens group is added between the lens groups may be used. The lens group is a portion having at least one lens separated by the aperture stop S as described above, or at least one piece separated by an air interval that changes at the time of zooming or focusing. The part which has a lens is shown.

  In this embodiment, the entire (all groups) feed is used to focus on an object at a short distance from an object at infinity. A focusing lens group that performs focusing from an object to a short-distance object may be used. That is, a method using the front group GF or a rear focus using the rear group GR may be used. In this case, the focusing lens group can be applied to autofocus, and is also suitable for driving a motor for autofocus (using an ultrasonic motor or the like).

  Also, by moving the lens group or partial lens group so that it has a component in the direction perpendicular to the optical axis, or rotating (swinging) in the in-plane direction including the optical axis, image blur caused by camera shake is corrected. An anti-vibration lens group may be used. In particular, it is preferable that at least one of the rear group GR is an anti-vibration lens group.

  Further, the lens surface may be formed as a spherical surface, a flat surface, or an aspheric surface. It is preferable that the lens surface is a spherical surface or a flat surface because lens processing and assembly adjustment are facilitated, and deterioration of optical performance due to errors in processing and assembly adjustment is prevented. Further, even when the image plane is shifted in the optical axis direction, it is preferable because there is little deterioration in the drawing performance. When the lens surface is an aspheric surface, the aspheric surface is an aspheric surface by grinding, a glass mold aspheric surface made of glass with an aspheric shape, or a composite aspheric surface made of resin on the glass surface. Any of the aspherical surfaces may be used. The lens surface may be a diffractive surface, and the lens may be a gradient index lens (GRIN lens) or a plastic lens.

  The aperture stop S is preferably arranged near the center of the optical system OS. However, the role of the aperture stop may be substituted by a lens frame without providing a member as an aperture stop.

  Further, each lens surface may be provided with an antireflection film having a high transmittance in a wide wavelength range in order to reduce flare and ghost and achieve high optical performance with high contrast.

  Hereinafter, an outline of a method for manufacturing the optical system OS according to the present embodiment will be described with reference to FIG. In this method of manufacturing the optical system OS, the front group GF and the rear group GR having a positive refractive power are arranged in this order from the object side along the optical axis. Specifically, in the present embodiment, for example, as the front group GF, in order from the object side, a biconvex lens-shaped aspherical positive lens L11 (first positive lens component LFP), which has a negative refractive power, A negative meniscus lens L12 (second lens component LFN1) having a convex surface and a biconcave lens L13 (third lens component LFN2) having negative refractive power are disposed (step S100), and the rear group GR is formed from the object side. In order, the biconcave lens L21 and the biconvex lens L22 are cemented, the first lens component LRN having a concave surface facing the object side, the biconvex lens L23 and the biconcave lens L24 are cemented, and has a positive refractive power as a whole, and the image A second lens component LRP1 having a concave surface facing the side and a biconvex lens-shaped aspherical positive lens L25 having a positive refractive power (third lens component LRP2) are disposed (step S200). . At this time, the first lens component LRN and the second lens component LRP1 constituting the rear group GR satisfy the above-described conditional expressions (1) and (2).

  As described above, according to the optical system OS according to the present embodiment, a small and high-performance lens suitable for an imaging device such as a camera, a printing lens, and a copying lens, and an imaging device using the same. Can be provided.

  Hereinafter, embodiments of the optical system OS will be described with reference to the drawings. 1, 3, 5, 7, 9, 11, 13, and 15 illustrate the configuration of the optical system OS (OS1 to OS8) according to each embodiment.

In each embodiment, the height of the aspheric surface in the direction perpendicular to the optical axis is y, and the distance (sag amount) along the optical axis from the tangential plane of the apex of each aspheric surface to each aspheric surface at height y. Is S (y), r is the radius of curvature of the reference sphere (paraxial radius of curvature), κ is the conic constant, and An is the nth-order aspherical coefficient, and is expressed by the following equation (a). . In the following examples, “E−n” indicates “× 10 ⁻ⁿ ”.

S (y) = (y ² / r) / [1+ {1−κ (y ² / r ² )} ^1/2 ]
+ A4 × y ⁴ + A6 × y ⁶ + A8 × y ⁸ + A10 × y ¹⁰ (a)

  In each embodiment, the secondary aspheric coefficient A2 is zero. In the table of each example, an aspherical surface is marked with * on the right side of the surface number.

[First embodiment]
FIG. 1 is a diagram illustrating a configuration of an optical system OS1 according to the first example. The optical system OS1 includes, in order from the object side, a front group GF having a positive refractive power, an aperture stop S, and a rear group GR having a positive refractive power. The front group GF includes, in order from the object side, a first lens component LFP including a biconvex aspherical positive lens L11, a second lens component LFN1 including a negative meniscus lens L12 having a convex surface facing the object side, and a biconcave lens. The third lens component LFN2 is composed of L13. In the rear group GR, in order from the object side, a biconcave lens (negative lens) L21 and a biconvex lens (positive lens) L22 are cemented, and a first lens component LRN having a concave surface facing the object side, a biconvex lens (positive lens) ) L23 and a biconcave lens (negative lens) L24 are cemented, and from the second lens component LRP1 having a positive refractive power as a whole and having a concave surface facing the image side, and a biconvex aspherical positive lens L25 The third lens component LRP2 is formed. A dummy glass FL corresponding to an optical low-pass filter is disposed between the rear group GR of the optical system OS1 and the image plane.

  Table 1 below lists values of specifications of the optical system OS1 according to the first example. In the overall specifications of Table 1, f is the focal length, FNO is the F number, ω is the half angle of view (unit: degree), Y is the image height, TL is the total length of the optical system OS1, and Bf is the back focus. Represents each. The total length TL indicates the distance on the optical axis from the most object side lens surface (first surface) of the optical system OS1 to the image plane, and the air conversion back focus Bf is obtained when the dummy glass FL is removed. This represents the distance on the optical axis from the most image side lens surface (fifteenth surface) of the optical system OS1 to the image surface. In the lens data, the first column m indicates the order (surface number) of the optical surfaces from the object side along the traveling direction of the light beam, the second column r indicates the curvature radius of each optical surface, The column d shows the distance (surface interval) on the optical axis from each optical surface to the next optical surface, and the fourth column νd and the fifth column nd show the Ab for the d-line (wavelength λ = 587.6 nm), respectively. Number and refractive index are shown. The surface numbers 1 to 17 shown in Table 1 correspond to the numbers 1 to 17 shown in FIG. A curvature radius of 0.0000 indicates a plane on the lens surface and an aperture on the aperture stop S. Further, the refractive index of air of 1.0000 is omitted. Further, the surface interval of the final surface (the 17th surface) is a distance on the optical axis to the image surface. The lens group focal length indicates the surface number (starting surface) where each lens group starts and the focal length of each lens group.

  Here, the focal length f, the radius of curvature r, the surface interval d, and other length units listed in all the following specification values are generally “mm”, but the optical system is proportionally enlarged or proportional. Since the same optical performance can be obtained even if the image is reduced, the present invention is not limited to this. The description of these symbols and the description of the specification table are the same in the following embodiments.

(Table 1)
[Overall specifications]
f = 58.0220
FNO = F1.210
ω = 20.81 °
Y = 21.6
TL = 108.8935
Air equivalent Bf = 38.0120

[Lens data]
m rd νd nd
1 * 65.8839 7.0000 49.53 1.744430
2 -497.8249 0.1000
3 31.8477 8.0000 63.88 1.516800
4 25.3357 7.5000
5 -1352.9378 1.5000 31.16 1.688930
6 45.3369 5.5000
7 0.0000 8.5000 Aperture stop S
8 -26.2017 1.7000 29.57 1.717360
9 140.0354 9.8000 46.59 1.816000
10 -37.7310 0.1000
11 40.8209 10.0000 49.62 1.772500
12 -155.3245 1.3000 41.51 1.575010
13 32.9483 2.7000
14 54.6222 6.5000 49.53 1.744430
15 * -117.5302 36.0000
16 0.0000 2.0000 63.88 1.516800
17 0.0000 0.6935

[Lens focal length]
Lens group Start surface Focal length Front group 1 1452.0656
Rear group 8 41.4561

  In the optical system OS1 according to the first example, each lens surface of the first surface and the fifteenth surface is formed in an aspherical shape. Table 2 below shows the aspheric data, that is, the values of the conic constant κ and the aspheric constants A4 to A6. The aspheric constants (A8 to A10) that are not displayed are 0 (the same applies to the following examples).

(Table 2)
κ A4 A6
First side -0.4179 6.27748E-08 -9.11068E-11
15th 3.6628 2.28024E-06 7.37001E-10

  Table 3 below shows values corresponding to the conditional expressions for the optical system OS1 according to the first example. In Table 3, nRNP is the refractive index with respect to the d-line of the medium of the positive lens L22 in the first lens component LRN in the rear group GR, and nRNN is the negative lens L21 in the first lens component LRN in the rear group GR. Rp1 is the radius of curvature of the most object side surface of the second lens component LRP1 in the rear group GR, and rp2 is the most image side surface of the second lens component LRP1 in the rear group GR. The radius of curvature, fFN1 is the focal length of the second lens component LFN1 in the front group GF, fFN2 is the focal length of the third lens component LFN2 in the front group GF, and nRPP is the positive lens of the second lens component LRP1 in the rear group GR. The refractive index with respect to the d-line of the medium of L23, nRPN: is the refractive index of the second lens component LRP1 in the group GR with respect to the d-line of the medium of the negative lens L24, and fRP is the second lens component LRP in the rear group GR. The focal length of, FRP third lens focal length components LRP2 in the rear group GR is, f0 is the focal length of the entire system when focused on an object at infinity, respectively. The description of these symbols is the same in the following embodiments.

(Table 3)
(1) nRNP-nRNN = 0.09864
(2) (rp2-rp1) / (rp2 + rp1) = − 0.1067
(3) (-fFN1) /f0=7.1072
(4) (−fFN2) /f0=1.0970
(5) nRPP-nRPN = 0.1975
(6) fRP / f0 = 3.6208
(7) fRP2 / f0 = 0.8775

  Thus, the optical system OS1 according to the first example satisfies all the conditional expressions (1) to (7).

  FIG. 2 shows various aberration diagrams of spherical aberration, astigmatism, distortion aberration, lateral chromatic aberration, and coma aberration in the infinitely focused state of the optical system OS1 according to the first example. In each aberration diagram, FNO represents an F number, Y represents an image height, and ω represents a half angle of view [unit: degree]. In each aberration diagram, d represents the aberration with respect to the d-line (wavelength λ = 587.6 nm), and g represents the aberration with respect to the g-line (wavelength λ = 435.8 nm). In the astigmatism diagram, the solid line indicates the sagittal image plane, and the broken line indicates the meridional image plane. In the coma aberration diagram, at each half angle of view ω, the solid line represents the meridional coma aberration with respect to the d-line and the g-line, and the broken line on the left side from the origin represents the sagittal coma aberration generated in the meridional direction with respect to the d-line. The broken line represents the sagittal coma generated in the sagittal direction with respect to the d line. The description of this aberration diagram is the same in the following examples. As is apparent from the respective aberration diagrams shown in FIG. 2, in the optical system OS1 according to the first example, various aberrations including spherical aberration, sagittal coma, field curvature, astigmatism, and meridional coma are corrected well. It can be seen that it has high optical performance.

[Second Embodiment]
FIG. 3 is a diagram illustrating a configuration of the optical system OS2 according to the second embodiment. The optical system OS2 includes, in order from the object side, a front group GF having a positive refractive power, an aperture stop S, and a rear group GR having a positive refractive power. The front group GF includes, in order from the object side, a first lens component LFP including a biconvex aspherical positive lens L11, a positive meniscus lens L12 having a convex surface on the object side, and a negative meniscus lens L13 having a convex surface on the object side. And a second lens component LFN1 having a negative meniscus lens shape as a whole and a third lens component LFN2 including a biconcave lens L14. In the rear group GR, in order from the object side, a biconcave lens (negative lens) L21 and a biconvex lens (positive lens) L22 are cemented, and a first lens component LRN having a concave surface facing the object side, a biconvex lens (positive lens) ) L23 and a biconcave lens (negative lens) L24 are cemented, and from the second lens component LRP1 having a positive refractive power as a whole and having a concave surface facing the image side, and a biconvex aspherical positive lens L25 The third lens component LRP2 is formed. A dummy glass FL corresponding to an optical low-pass filter is disposed between the rear group GR of the optical system OS2 and the image plane.

  Table 4 below lists values of specifications of the optical system OS2 according to the second example. In addition, the surface numbers 1-18 shown in this Table 4 respond | correspond to the numbers 1-18 shown in FIG.

(Table 4)
[Overall specifications]
f = 58.0216
FNO = F1.210
ω = 21.03 °
Y = 21.6
TL = 111.4017
Air conversion Bf = 38.0203

[Lens data]
m rd νd nd
1 * 48.5419 9.0000 49.53 1.744430
2 -4006.7159 0.1000
3 41.2667 6.5000 82.57 1.497820
4 60.0000 1.5000 63.88 1.516800
5 24.7856 7.5000
6 -11889.5204 1.5000 31.16 1.688930
7 45.6954 5.5000
8 0.0000 8.5000 Aperture stop S
9 -26.7890 1.7000 29.57 1.717360
10 95.9330 9.8000 46.59 1.816000
11 -40.5577 0.1000
12 40.7407 10.0000 49.62 1.772500
13 -352.6242 1.3000 41.51 1.575010
14 32.8034 2.7000
15 51.7528 7.0000 49.53 1.744430
16 * -90.7205 36.0000
17 0.0000 2.0000 63.88 1.516800
18 0.0000 0.7017

[Lens focal length]
Lens group Start surface Focal length Front group 1 4379.4722
Rear group 9 40.0599

  In the optical system OS2 according to the second example, the first and sixteenth lens surfaces are formed in an aspherical shape. Table 5 below shows the aspheric data, that is, the values of the conic constant κ and the aspheric constants A4 to A6.

(Table 5)
κ A4 A6
1st surface -0.0458 2.67968E-07 -1.70729E-10
16th 1.9662 2.63114E-06 1.81677E-10

  Table 6 below shows values corresponding to the conditional expressions for the optical system OS2 according to the second example.

(Table 6)
(1) nRNP-nRNN = 0.09864
(2) (rp2-rp1) / (rp2 + rp1) = − 0.1079
(3) (-fFN1) /f0=2.4136
(4) (−fFN2) /f0=1.1388
(5) nRPP-nRPN = 0.1975
(6) fRP / f0 = 4.2148
(7) fRP2 / f0 = 0.7793

  Thus, the optical system OS2 according to the second example satisfies all the conditional expressions (1) to (7).

  FIG. 4 shows various aberration diagrams of spherical aberration, astigmatism, distortion aberration, lateral chromatic aberration, and coma aberration in the infinitely focused state of the optical system OS2 according to the second example. As is apparent from the respective aberration diagrams shown in FIG. 4, in the optical system OS2 according to the second example, various aberrations including spherical aberration, sagittal coma, field curvature, astigmatism, and meridional coma are corrected well. It can be seen that it has high optical performance.

[Third embodiment]
FIG. 5 is a diagram illustrating a configuration of the optical system OS3 according to the third embodiment. The optical system OS3 includes, in order from the object side, a front group GF having a positive refractive power, an aperture stop S, and a rear group GR having a positive refractive power. The front group GF includes, in order from the object side, a first lens component LFP composed of an aspheric positive lens L11 having a biconvex lens shape, a second lens component LFN1 composed of a negative meniscus lens L12 having a convex surface facing the object side, and the object side. The third lens component LFN2 is composed of a negative meniscus lens L13 having a convex surface facing the surface. In the rear group GR, in order from the object side, a biconcave lens (negative lens) L21 and a biconvex lens (positive lens) L22 are cemented, a first lens component LRN having a concave surface facing the object side, and a convex surface facing the object side. A positive meniscus lens (positive lens) L23 directed to a negative meniscus lens (negative lens) L24 having a convex surface facing the object side is cemented, and has a positive refractive power as a whole, and a second surface having a concave surface directed to the image side. It is composed of a lens component LRP1 and a third lens component LRP2 composed of a biconvex aspherical positive lens L25. A dummy glass FL corresponding to an optical low-pass filter is disposed between the rear group GR of the optical system OS3 and the image plane.

  Table 7 below provides values of specifications of the optical system OS3 according to the third example. The surface numbers 1 to 17 shown in Table 7 correspond to the numbers 1 to 17 shown in FIG.

(Table 7)
[Overall specifications]
f = 58.0216
FNO = F1.212
ω = 20.67 °
Y = 21.6
TL = 111.7529
Air equivalent Bf = 38.0715

[Lens data]
m rd νd nd
1 * 42.9001 9.0000 49.53 1.744430
2 -759.7809 0.1000
3 39.3381 5.0000 63.88 1.516800
4 23.0671 7.0000
5 109.0084 1.5000 31.16 1.688930
6 30.0146 7.5000
7 0.0000 8.5000 Aperture stop S
8 -29.9941 1.7000 29.57 1.717360
9 53.7056 12.0000 46.59 1.816000
10 -39.1782 0.1000
11 35.1890 7.0000 52.34 1.755000
12 141.3160 1.3000 45.51 1.548140
13 28.5039 4.8000
14 72.7463 7.5000 49.53 1.744430
15 * -87.9348 36.0000
16 0.0000 2.0000 63.88 1.516800
17 0.0000 0.7529

[Lens focal length]
Lens group Start surface Focal length Front group 1 2966.21728
Rear group 8 41.35903

  In the optical system OS3 according to the third example, each lens surface of the first surface and the fifteenth surface is formed in an aspherical shape. Table 8 below shows the aspheric data, that is, the values of the conic constant κ and the aspheric constants A4 to A6.

(Table 8)
κ A4 A6
First side -0.2253 1.10855E-07 -5.77849E-10
15th 3.8248 1.40952E-06 -1.06066E-10

  Table 9 below shows values corresponding to the conditional expressions for the optical system OS3 according to the third example.

(Table 9)
(1) nRNP-nRNN = 0.09864
(2) (rp2-rp1) / (rp2 + rp1) = − 0.1050
(3) (−fFN1) /f0=2.0774
(4) (−fFN2) /f0=1.0443
(5) nRPP-nRPN = 0.2069
(6) fRP / f0 = 6.0322
(7) fRP2 / f0 = 0.9405

  Thus, the optical system OS3 according to the third example satisfies all the conditional expressions (1) to (7).

  FIG. 6 shows various aberration diagrams of spherical aberration, astigmatism, distortion aberration, lateral chromatic aberration, and coma aberration in the infinite focus state of the optical system OS3 according to the third example. As is apparent from each aberration diagram shown in FIG. 6, in the optical system OS3 according to the third example, various aberrations including spherical aberration, sagittal coma, field curvature, astigmatism, and meridional coma are corrected well. It can be seen that it has high optical performance.

[Fourth embodiment]
FIG. 7 is a diagram illustrating a configuration of an optical system OS4 according to the fourth example. The optical system OS4 includes, in order from the object side, a front group GF having a positive refractive power, an aperture stop S, and a rear group GR having a positive refractive power. The front group GF includes, in order from the object side, a first lens component LFP composed of an aspheric positive lens L11 having a biconvex lens shape, a second lens component LFN1 composed of a negative meniscus lens L12 having a convex surface facing the object side, and the object side. The third lens component LFN2 is composed of a negative meniscus lens L13 having a convex surface facing the surface. In the rear group GR, in order from the object side, a biconcave lens (negative lens) L21 and a biconvex lens (positive lens) L22 are cemented, a first lens component LRN having a concave surface facing the object side, and a convex surface facing the object side. A positive meniscus lens (positive lens) L23 directed to a negative meniscus lens (negative lens) L24 having a convex surface facing the object side is cemented, and has a positive refractive power as a whole, and a second surface having a concave surface directed to the image side. It is composed of a lens component LRP1 and a third lens component LRP2 composed of a biconvex aspherical positive lens L25. A dummy glass FL corresponding to an optical low-pass filter is disposed between the rear group GR of the optical system OS4 and the image plane.

  Table 10 below lists values of specifications of the optical system OS4 according to the fourth example. The surface numbers 1 to 17 shown in Table 10 correspond to the numbers 1 to 17 shown in FIG.

(Table 10)
[Overall specifications]
f = 58.0216
FNO = F1.2075
ω = 20.71 °
Y = 21.6
TL = 115.1080
Air conversion Bf = 38.2266

[Lens data]
m rd νd nd
1 * 42.3307 11.0000 49.53 1.744430
2 -1195.5447 0.1000
3 38.4586 3.0000 63.88 1.516800
4 22.9860 9.0000
5 100.1795 1.5000 31.16 1.688930
6 30.4674 7.0000
7 0.0000 8.5000 Aperture stop S
8 -28.6498 1.7000 29.57 1.717360
9 56.2750 13.0000 46.59 1.816000
10 -38.4062 0.1000
11 36.0036 8.5000 49.62 1.772500
12 147.7696 1.3000 41.51 1.575010
13 28.8771 5.0000
14 65.3476 6.5000 49.53 1.744430
15 * -98.9846 36.0000
16 0.0000 2.0000 63.88 1.516800
17 0.0000 0.9080

[Lens focal length]
Lens group Start surface Focal length Front group 1 2657.53882
Rear group 8 41.38318

  In the optical system OS4 according to the fourth example, each lens surface of the first surface and the fifteenth surface is formed in an aspherical shape. Table 11 below shows the aspheric data, that is, the values of the conic constant κ and the aspheric constants A4 to A6.

(Table 11)
κ A4 A6
1st surface -0.2144 3.20826E-07 -5.21258E-10
Surface 15 1.9946 1.02179E-06 -1.79192E-10

  Table 12 below shows values corresponding to the conditional expressions for the optical system OS4 according to the fourth example.

(Table 12)
(1) nRNP-nRNN = 0.09864
(2) (rp2-rp1) / (rp2 + rp1) = − 0.1098
(3) (-fFN1) /f0=2.0402
(4) (-fFN2) /f0=1.1050
(5) nRPP-nRPN = 0.1975
(6) fRP / f0 = 6.3210
(7) fRP2 / f0 = 0.9270

  As described above, the optical system OS4 according to the fourth example satisfies all the conditional expressions (1) to (7).

  FIG. 8 shows various aberration diagrams of spherical aberration, astigmatism, distortion aberration, lateral chromatic aberration, and coma aberration in the infinitely focused state of the optical system OS4 according to the fourth example. As is apparent from the aberration diagrams shown in FIG. 8, in the optical system OS4 according to the fourth example, various aberrations including spherical aberration, sagittal coma, field curvature, astigmatism, and meridional coma are corrected well. It can be seen that it has high optical performance.

[Fifth embodiment]
FIG. 9 is a diagram illustrating a configuration of an optical system OS5 according to the fifth example. The optical system OS5 includes, in order from the object side, a front group GF having a positive refractive power, an aperture stop S, and a rear group GR having a positive refractive power. The front group GF includes, in order from the object side, a first lens component LFP including a biconvex aspherical positive lens L11, a positive meniscus lens L12 having a convex surface on the object side, and a negative meniscus lens L13 having a convex surface on the object side. And a second lens component LFN1 having a negative meniscus lens shape as a whole, and a third lens component LFN2 including a negative meniscus lens L14 having a convex surface facing the object side. In the rear group GR, in order from the object side, a biconcave lens (negative lens) L21 and a biconvex lens (positive lens) L22 are cemented, a first lens component LRN having a concave surface facing the object side, and a convex surface facing the object side. A positive meniscus lens (positive lens) L23 directed to a negative meniscus lens (negative lens) L24 having a convex surface facing the object side is cemented, and has a positive refractive power as a whole, and a second surface having a concave surface directed to the image side. It is composed of a lens component LRP1 and a third lens component LRP2 composed of a biconvex aspherical positive lens L25. A dummy glass FL corresponding to an optical low-pass filter is disposed between the rear group GR of the optical system OS5 and the image plane.

  Table 13 below provides values of specifications of the optical system OS5 according to the fifth example. The surface numbers 1 to 18 shown in Table 13 correspond to the numbers 1 to 18 shown in FIG.

(Table 13)
[Overall specifications]
f = 58.0216
FNO = F1.210
ω = 20.81 °
Y = 21.6
TL = 110.39748
Air conversion Bf = 38.01604

[Lens data]
m rd νd nd
1 * 49.8688 9.0000 49.53 1.744430
2 -518.0363 0.1000
3 40.2883 5.5000 52.20 1.517420
4 60.0000 1.5000 63.88 1.516800
5 27.9254 6.0000
6 168.7999 1.5000 31.16 1.688930
7 30.2735 7.5000
8 0.0000 8.5000 Aperture stop S
9 -28.8341 1.7000 29.57 1.717360
10 78.5900 10.5000 46.59 1.816000
11 -40.5395 0.1000
12 37.3064 7.5000 49.62 1.772500
13 396.2828 1.3000 41.51 1.575010
14 30.5026 4.0000
15 62.3814 7.0000 49.53 1.744430
16 * -82.5179 36.0000
17 0.0000 2.0000 63.88 1.516800
18 0.0000 0.6975

[Lens focal length]
Lens group Start surface Focal length Front group 1 2115.41898
Rear group 9 40.65448

  In the optical system OS5 according to the fifth example, the lens surfaces of the first surface and the sixteenth surface are formed in an aspherical shape. Table 14 below shows the aspheric data, that is, the values of the conic constant κ and the aspheric constants A4 to A6.

(Table 14)
κ A4 A6
1st surface -0.2362 3.22585E-08 -4.00333E-10
16th 2.6137 1.95398E-06 -1.27860E-10

  Table 15 below shows values corresponding to the conditional expressions for the optical system OS5 according to the fifth example.

(Table 15)
(1) nRNP-nRNN = 0.09864
(2) (rp2-rp1) / (rp2 + rp1) = − 0.1003
(3) (-fFN1) /f0=3.7656
(4) (−fFN2) /f0=0.9270
(5) nRPP-nRPN = 0.1975
(6) fRP / f0 = 5.1177
(7) fRP2 / f0 = 0.8398

  Thus, the optical system OS5 according to the fifth example satisfies all the conditional expressions (1) to (7).

  FIG. 10 shows various aberration diagrams of spherical aberration, astigmatism, distortion aberration, lateral chromatic aberration, and coma aberration in the infinitely focused state of the optical system OS5 according to the fifth example. As is apparent from the aberration diagrams shown in FIG. 10, in the optical system OS5 according to the fifth example, various aberrations including spherical aberration, sagittal coma, field curvature, astigmatism, and meridional coma are corrected well. It can be seen that it has high optical performance.

[Sixth embodiment]
FIG. 11 is a diagram illustrating a configuration of an optical system OS6 according to the sixth example. The optical system OS6 includes, in order from the object side, a front group GF having a positive refractive power, an aperture stop S, and a rear group GR having a positive refractive power. In the front group GF, in order from the object side, a first lens component LFP including a positive meniscus aspherical positive lens L11 having a convex surface directed toward the object side, a biconvex lens L12, and a biconcave lens L13 are cemented and negative as a whole. A second lens component LFN1 having a meniscus lens shape and a third lens component LFN2 including a negative meniscus lens L14 having a concave surface facing the object side. In the rear group GR, in order from the object side, a biconcave lens (negative lens) L21 and a biconvex lens (positive lens) L22 are cemented, and a first negative lens component LRN having a concave surface facing the object side, a biconvex lens (positive) Lens) L23 and biconcave lens (negative lens) L24 are cemented, and have a positive refracting power as a whole, a second lens component LRP1 having a concave surface facing the image side, and a biconvex aspherical positive lens L25 Is composed of a third lens component LRP2. A dummy glass FL equivalent to an optical low-pass filter is disposed between the rear group GR of the optical system OS6 and the image plane.

  Table 16 below provides values of specifications of the optical system OS6 according to the sixth example. In addition, the surface numbers 1-18 shown in this Table 16 respond | correspond to the numbers 1-18 shown in FIG.

(Table 16)
[Overall specifications]
f = 58.0216
FNO = F1.229
ω = 20.82 °
Y = 21.6
TL = 122.05004
Air conversion Bf = 38.01861

[Lens data]
m rd νd nd
1 * 41.8098 11.0500 49.53 1.744430
2 * 2652.8412 1.0000
3 117.6517 5.4000 82.57 1.497820
4 -257.3631 1.5000 48.78 1.531720
5 22.4645 11.0000
6 -55.6445 2.0000 70.31 1.487490
7 -96.0152 3.0000
8 0.0000 10.0000 Aperture stop S
9 -29.5135 1.7000 28.38 1.728250
10 109.6394 11.0000 46.59 1.816000
11 -40.5171 0.1000
12 44.9154 14.5000 49.62 1.772500
13 -50.7224 1.6000 41.51 1.575010
14 33.7818 2.5000
15 54.2656 7.0000 49.53 1.744430
16 * -233.5493 36.0000
17 0.0000 2.0000 63.88 1.516800
18 0.0000 0.7000

[Lens focal length]
Lens group Start surface Focal length Front group 1 6928.27452
Rear group 9 43.40473

  In the optical system OS6 according to the sixth example, the lens surfaces of the first surface, the second surface, and the sixteenth surface are formed in an aspherical shape. Table 17 below shows the aspheric data, that is, the values of the conic constant κ and the aspheric constants A4 to A10.

(Table 17)
κ A4 A6 A8 A10
First side -1.3241 3.10229E-06 -7.79759E-10 3.01550E-13 -7.29996E-16
2nd surface -0.1653E + 05 -7.21606E-08 7.08003E-11 -3.55610E-13 1.07080E-17
16th surface -16.7337 1.90857E-06 4.23655E-09 -1.20892E-11 2.56021E-14

  Table 18 below shows values corresponding to the conditional expressions for the optical system OS6 according to the sixth example.

(Table 18)
(1) nRNP-nRNN = 0.08775
(2) (rp2-rp1) / (rp2 + rp1) = − 0.1415
(3) (−fFN1) /f0=0.9018
(4) (−fFN2) /f0=4.7562
(5) nRPP-nRPN = 0.1975
(6) fRP / f0 = 2.7473
(7) fRP2 / f0 = 1.0302

  As described above, the optical system OS6 according to the sixth example satisfies all the conditional expressions (1) to (7).

  FIG. 12 shows various aberration diagrams of spherical aberration, astigmatism, distortion aberration, lateral chromatic aberration, and coma aberration in the infinitely focused state of the optical system OS6 according to the sixth example. As is apparent from the respective aberration diagrams shown in FIG. 12, in the optical system OS6 according to the sixth example, various aberrations including spherical aberration, sagittal coma, field curvature, astigmatism, and meridional coma are corrected well. It can be seen that it has high optical performance.

[Seventh embodiment]

  FIG. 13 is a diagram illustrating a configuration of an optical system OS7 according to the seventh example. The optical system OS7 includes, in order from the object side, a front group GF having a positive refractive power, an aperture stop S, and a rear group GR having a positive refractive power. In the front group GF, in order from the object side, a first lens component LFP including a positive meniscus aspherical positive lens L11 having a convex surface directed toward the object side, a biconvex lens L12, and a biconcave lens L13 are cemented and negative as a whole. A second lens component LFN1 having a meniscus lens shape and a third lens component LFN2 including a negative meniscus lens L14 having a concave surface facing the object side. In the rear group GR, in order from the object side, a biconcave lens (negative lens) L21 and a biconvex lens (positive lens) L22 are cemented, and a first negative lens component LRN having a concave surface facing the object side, a biconvex lens (positive) Lens) L23 and biconcave lens (negative lens) L24 are cemented, and have a positive refracting power as a whole, a second lens component LRP1 having a concave surface facing the image side, and a biconvex aspherical positive lens L25 Is composed of a third lens component LRP2. A dummy glass FL corresponding to an optical low-pass filter is disposed between the rear group GR of the optical system OS7 and the image plane.

  Table 19 below provides values of specifications of the optical system OS7 according to the seventh example. The surface numbers 1 to 18 shown in Table 19 correspond to the numbers 1 to 18 shown in FIG.

(Table 19)
[Overall specifications]
f = 58.0216
FNO = F1.2300
ω = 20.83 °
Y = 21.6
TL = 121.55017
Air conversion Bf = 38.01873

[Lens data]
m rd νd nd
1 * 42.3882 11.0500 49.53 1.744430
2 * 2167.3376 1.0000
3 113.8826 5.4000 82.57 1.497820
4 -622.3931 1.5000 48.78 1.531720
5 22.7071 11.0000
6 -60.3750 2.0000 52.20 1.517420
7 -96.0594 3.0000
8 0.0000 10.0000 Aperture stop S
9 -28.9264 1.7000 28.38 1.728250
10 129.6692 11.0000 46.59 1.816000
11 -39.3334 0.1000
12 46.0594 14.0000 49.62 1.772500
13 -50.2692 1.6000 41.51 1.575010
14 34.3180 2.5000
15 55.6965 7.0000 49.53 1.744430
16 * -232.9169 36.0000
17 0.0000 2.0000 63.88 1.516800
18 0.0000 0.7002

[Lens focal length]
Lens group Start surface Focal length Front group 1 1869.98022
Rear group 9 43.86208

  In the optical system OS7 according to the seventh example, the lens surfaces of the first surface, the second surface, and the sixteenth surface are formed in an aspherical shape. Table 20 below shows the aspheric data, that is, the values of the conic constant κ and the aspheric constants A4 to A10.

(Table 20)
κ A4 A6 A8 A10
1st surface -1.3412 2.99857E-06 -8.24891E-10 2.35245E-13 -4.91290E-16
2nd surface -0.3444E + 04 -8.68033E-08 4.62357E-11 -2.08722E-13 -2.01437E-17
16th surface -8.6128 1.92924E-06 2.40259E-09 -6.72709E-12 1.77887E-14

  Table 21 below shows values corresponding to the conditional expressions for the optical system OS7 according to the seventh example.

(Table 21)
(1) nRNP-nRNN = 0.08775
(2) (rp2-rp1) / (rp2 + rp1) =-0.1461
(3) (−fFN1) /f0=0.9251
(4) (−fFN2) /f0=5.5192
(5) nRPP-nRPN = 0.1975
(6) fRP / f0 = 2.8784
(7) fRP2 / f0 = 1.0515

  As described above, the optical system OS7 according to the seventh example satisfies all the conditional expressions (1) to (7).

  FIG. 14 shows various aberration diagrams of spherical aberration, astigmatism, distortion aberration, lateral chromatic aberration, and coma aberration in the infinitely focused state of the optical system OS7 according to the seventh example. As is apparent from the aberration diagrams shown in FIG. 14, in the optical system OS7 according to the seventh example, various aberrations including spherical aberration, sagittal coma, field curvature, astigmatism, and meridional coma are corrected well. It can be seen that it has high optical performance.

[Eighth embodiment]
FIG. 15 is a diagram illustrating a configuration of an optical system OS8 according to the eighth example. The optical system OS8 includes, in order from the object side, a front group GF having a positive refractive power, an aperture stop S, and a rear group GR having a positive refractive power. In the front group GF, in order from the object side, a first lens component LFP including a positive meniscus aspherical positive lens L11 having a convex surface directed toward the object side, a biconvex lens L12, and a biconcave lens L13 are cemented and negative as a whole. A second lens component LFN1 having a meniscus lens shape and a third lens component LFN2 including a negative meniscus lens L14 having a concave surface facing the object side. In the rear group GR, in order from the object side, a biconcave lens (negative lens) L21 and a biconvex lens (positive lens) L22 are cemented, and a first positive lens component LRN having a concave surface facing the object side, a biconvex lens (positive) Lens) L23 and biconcave lens (negative lens) L24 are cemented, and have a positive refracting power as a whole, a second lens component LRP1 having a concave surface facing the image side, and a biconvex aspherical positive lens L25 Is composed of a third lens component LRP2. A dummy glass FL corresponding to an optical low-pass filter is disposed between the rear group GR of the optical system OS1 and the image plane.

  Table 22 below presents values of specifications of the optical system OS8 according to the eighth example. In addition, the surface numbers 1-18 shown in this Table 22 respond | correspond to the numbers 1-18 shown in FIG.

(Table 22)
[Overall specifications]
f = 58.0216
FNO = F1.2300
ω = 20.82 °
Y = 21.6
TL = 118.89463
Air equivalent Bf = 38.01320

[Lens data]
m rd νd nd
1 * 39.7073 11.0000 49.53 1.744430
2 * 2526.2002 0.1000
3 102.0678 6.5000 82.57 1.497820
4 -84.0848 1.5000 52.20 1.517420
5 21.4694 11.0000
6 -62.0246 2.0000 31.16 1.688930
7 -97.3881 3.0000
8 0.0000 10.0000 Aperture stop S
9 -26.3978 1.7000 29.57 1.717360
10 72.7424 12.0000 46.59 1.816000
11 -37.7187 0.1000
12 45.2189 10.0000 49.62 1.772500
13 -117.8426 1.3000 41.51 1.575010
14 33.4623 3.0000
15 56.4087 7.0000 49.53 1.744430
16 * -132.4054 36.0000
17 0.0000 2.0000 63.88 1.516800
18 0.0000 0.6946

[Lens focal length]
Lens group Start surface Focal length Front group 1 678.80939
Rear group 9 42.58204

  In the optical system OS8 according to the eighth example, the lens surfaces of the first surface, the second surface, and the sixteenth surface are formed in an aspherical shape. Table 23 below shows the aspheric data, that is, the values of the conic constant κ and the aspheric constants A4 to A10.

(Table 23)
κ A4 A6 A8 A10
First side -0.8567 3.05299E-06 -6.59016E-10 6.97421E-13 -4.05702E-16
2nd surface 0.5931E + 04 6.03268E-08 7.20986E-11 -2.17040E-13 8.89735E-17
16th surface 1.4374 1.57765E-06 -1.04169E-09 1.88087E-12 -4.58581E-16

  Table 24 below shows values corresponding to the conditional expressions for the optical system OS8 according to the eighth example.

(Table 24)
(1) nRNP-nRNN = 0.09864
(2) (rp2-rp1) / (rp2 + rp1) = − 0.1494
(3) (−fFN1) /f0=0.9153
(4) (−fFN2) /f0=4.3742
(5) nRPP-nRPN = 0.1975
(6) fRP / f0 = 5.1695
(7) fRP2 / f0 = 0.9306

  As described above, the optical system OS8 according to the eighth example satisfies all the conditional expressions (1) to (7).

  FIG. 16 shows various aberration diagrams of spherical aberration, astigmatism, distortion aberration, lateral chromatic aberration, and coma aberration in the infinitely focused state of the optical system OS8 according to the eighth example. As is apparent from the respective aberration diagrams shown in FIG. 16, in the optical system OS8 according to the eighth example, various aberrations including spherical aberration, sagittal coma, field curvature, astigmatism, and meridional coma are corrected well. It can be seen that it has high optical performance.

  According to each of the above-described embodiments, it has a comprehensive angle of about 2ω = 41.6 °, and further has a large aperture F1.2, high performance, spherical aberration, sagittal coma aberration, field curvature, meridional coma aberration. It is possible to realize an optical system OS in which is corrected well.

  Needless to say, the above-described effects can be obtained by mounting the optical systems OS1 to OS8 shown in the above embodiments in the camera 1 described above. Moreover, each said Example has shown the specific example of this invention, and this invention is not limited to these.

OS (OS1 to OS8) Optical system GF Front group LFP First lens component LFN1 Front lens second lens component LFN2 Front lens third lens component GR Rear group LRN Rear lens first lens component L21 Negative lens L22 Positive lens LRP1 Rear group second lens component L23 Positive lens L24 Negative lens LRP2 Rear group third lens component S Aperture stop 1 SLR camera (imaging device)

Claims (12)

In order from the object side along the optical axis,
The front group,
Consisting essentially of two lens groups with a rear group having positive refractive power,
The front group is in order from the object side,
A first lens component having a positive refractive power;
A second lens component having negative refractive power and having a convex surface facing the object side;
And a third lens component having a negative refractive power,
The rear group is in order from the object side,
A first lens component in which a negative lens and a positive lens are cemented and a concave surface is directed to the object side;
A second lens component having a positive refractive power and having a concave surface facing the image side;
And a third lens component having positive refractive power,
An optical system satisfying the following conditional expression:
0.000 <nRNP-nRNN <0.350
−2.00 <(rp2−rp1) / (rp2 + rp1) <− 0.00
However,
nRNP: Refractive index for the d-line of the medium of the positive lens in the first lens component in the rear group nRNN: Refractive index for the d-line of the medium of the negative lens in the first lens component in the rear group rp1: radius of curvature of the surface closest to the object side of the second lens component in the rear group rp2: radius of curvature of the surface closest to the image side of the second lens component in the rear group The optical system according to claim 1, wherein the following conditional expression is satisfied.
0.00 <(− fFN1) / f0 <20.00
However,
fFN1: focal length of the second lens component in the front group f0: focal length of the entire system when focusing on infinity The optical system according to claim 1, wherein the following conditional expression is satisfied.
0.20 <(-fFN2) / f0 <15.00
However,
fFN2: focal length of the third lens component in the front group f0: focal length of the entire system when focusing on infinity 4. The second lens component in the rear group is a cemented lens in which a positive lens and a negative lens are cemented, and satisfies the following conditional expression: 4. The optical system described in 1.
0.000 <nRPP-nRPN <0.500
However,
nRPP: refractive index of the second lens component in the rear group with respect to the d-line of the medium of the positive lens nRPN: refractive index of the second lens component in the rear group with respect to the d-line of the medium of the negative lens The optical system according to claim 1, wherein the following conditional expression is satisfied.
1.00 <fRP / f0 <12.00
However,
fRP: focal length of the second lens component in the rear group f0: focal length of the entire system when focusing on infinity The optical system according to claim 1, wherein the following conditional expression is satisfied.
0.1 <fRP2 / f0 <3.0
However,
fRP2: focal length of the third lens component in the rear group f0: focal length of the entire system when focusing on infinity   The optical system according to claim 1, wherein the front group has at least one aspheric surface.   The optical system according to claim 1, wherein the rear group has at least one aspheric surface.   The optical system according to any one of claims 1 to 8, wherein the third lens component in the rear group is a positive lens having a convex surface directed toward the object side.   The optical system according to claim 1, further comprising an aperture stop between the front group and the rear group.   An imaging apparatus comprising the optical system according to claim 1. In order from the object side along the optical axis, a manufacturing method of an optical system consisting essentially of two lens groups of a front group and a rear group having a positive refractive power,
As the front group, in order from the object side, a first lens component having a positive refractive power, a second lens component having a negative refractive power and having a convex surface facing the object side, and a first lens component having a negative refractive power. And three lens components,
As the rear group, in order from the object side, a negative lens and a positive lens are cemented, a first lens component having a concave surface facing the object side, a second lens having a positive refractive power and a concave surface facing the image side. A lens component and a third lens component having a positive refractive power,
An optical system manufacturing method satisfying the following conditional expression:
0.000 <nRNP-nRNN <0.350
−2.00 <(rp2−rp1) / (rp2 + rp1) <− 0.00
However,
nRNP: Refractive index for the d-line of the medium of the positive lens in the first lens component in the rear group nRNN: Refractive index for the d-line of the medium of the negative lens in the first lens component in the rear group rp1: radius of curvature of the surface closest to the object side of the second lens component in the rear group rp2: radius of curvature of the surface closest to the image side of the second lens component in the rear group

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